We perform simulations on a \(32^3 \times 6\)  lattice at \(\beta = 5.8810\)  and \(5.9000\) ,
and on a \(32^3 \times 8\)  lattice at \(\beta = 6.0320\)  and \(6.0660\) .
These \(\beta \)  values are chosen to be slightly below and above the phase transition point.The transition point determined by the peak of the Polyakov loop susceptibility locates at \(\beta _{\rm trans}=5.89383(24)\)  on a \(48^3\times 6\)  lattice and at \(6.06160(18)\)  on a \(48^3\times 8\)  lattice [1]}.
Details of the simulations are the same as in our previous studies [2]}, [3]}, [4]}, [5]}, [6]}.
Independent 50 configurations are generated at each \(\beta \) .
The number of noises \(N_{\rm noise}\)  is 1000 for each configuration.
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